diff --git a/Zurich_group/Mountain_hut_2015/QEE/mchrzasz.tex b/Zurich_group/Mountain_hut_2015/QEE/mchrzasz.tex
index 71239e6..be1d818 100644
--- a/Zurich_group/Mountain_hut_2015/QEE/mchrzasz.tex
+++ b/Zurich_group/Mountain_hut_2015/QEE/mchrzasz.tex
@@ -272,7 +272,7 @@
 \item $\PW$, $\PZ$ cross section.
 \item Drell-Yan cross section.
 \end{itemize}
-\item This measurements would strongly constrain the PDF in the fits.
+\item These measurements would strongly constrain the PDF in the fits.
 \end{itemize}
 
 
@@ -289,7 +289,7 @@
 
 \begin{frame}\frametitle{What could we do?}
 
-$\Rrightarrow$ For starters we should start by measurement of $\PZ$ cross section.\\
+$\Rrightarrow$ For starters we should start by measurement of $\PZ$ cross section (already ongoing in the group).\\
 $\Rightarrow$ Relativity simple, you don't need much data.\\
 $\Rightarrow$ Important for MC tuning.\\
 $\Rrightarrow$ More interesting: Tripple Gauge Boson Couplings:\\{~}\\
@@ -321,6 +321,7 @@
 \item Effectively you are probing the proton PDF. 
 \item Remember that the theory error for all the Higgs calculations comes from PDFs.
 \item One could improve really the PDFs thanks to special kinematic region of LHCb.
+\item We could reach lower $x$ region of $10^{-6}$, trigger is there! Background needs to be understood.
 \end{itemize}
 
 \column{0.5\textwidth}
@@ -342,6 +343,7 @@
 \item Super clean theoretically.
 \item Signature: protons interact and go to the beam pipe undetected, in the detector you are left with couple of particles.
 \item Probing PDF and also thanks to DPE we have a link to Higgs Physics.
+\item Getting sensitive to saturation effects?
 \end{itemize}
 
 \column{0.3\textwidth}
@@ -358,6 +360,8 @@
 \item For Run2 LHCb installed:HeRSCheL: High Rapidity Shower Counters 
 \item They cover $5<\eta<8$.
 \item Rejecting the main background for CEP.
+\item Allows to measure $p_T^2$ distribution for inelastic events.
+\item Dedicated \texttt{L0} trigger for CEP.
 \end{itemize}
 
 
@@ -399,7 +403,7 @@
 \begin{itemize}
 \item Competitive with ATLAS and CMS
 \item We have excellent resolution.
-\item Can problem mass around the $\Upsilon$s region.
+\item Can probe mass around the $\Upsilon$s region.
 \end{itemize}
 
 
@@ -432,6 +436,7 @@
 \item This is dependent on the vector and axial couplings $\Rightarrow$ $\sin \theta_W^{eff}$.
 \item Since LEP time there is a small tension in this measurement.
 \item With full Run2 data and some smart ideas we might be close to LEP!
+\item ATLAS and CMS will not not be able to compete.
 \end{itemize}
 
 \column{0.45\textwidth}
@@ -444,7 +449,7 @@
 
 \begin{frame}\frametitle{Summary}
 \begin{itemize}
-\item Reach Run2 program in Electroweak measurements:
+\item Reach Run2 program in QEE WG measurements:
 \begin{enumerate}
 \item Drell-Yan
 \item Ion-Ion physics